Determinant and energy identities for Higgs walls #
Polynomial identities, over any commutative ring, behind the analysis of Higgs walls in
six-dimensional gauge-Higgs unification: the rank-one wall determinant, the neutral 3 × 3
Gram determinant and its sum-of-squares decomposition, and the rationalized gap formula. They do
not formalize traces in H¹, the Robin boundary problem, the positivity of its spectrum or the
physical derivation of the input matrices.
Main results #
amplitude_circle:(p² − q²)² + (2pq)² = (p² + q²)²(the parametrization of Pythagorean triples; Mathlib'sPythagoreanTripleis stated overℤ).rank_one_wall_det:det [[a x², a x y], [a x y, a y² + b]] = a b x².gap_discriminant,gap_rationalization:(r + t − z)(r + t + z) = 4rt(1 − c)whenz² = (r − t)² + 4rtc.neutral_three_det: the neutral3 × 3Gram determinant isa b x² (k + a(1 − d²)).neutral_energy_decomposition: the corresponding quadratic form isa (x u + y v − d w)² + b v² + (k + a(1 − d²)) w².
The 2 × 2 determinant.
Equations
- GaugeHiggsUnification.WallDeterminants.det2 a b c d = a * d - b * c
Instances For
def
GaugeHiggsUnification.WallDeterminants.det3
{R : Type u_1}
[CommRing R]
(a b c d e f g h i : R)
:
R
The 3 × 3 determinant, expanded along the first row.
Equations
Instances For
theorem
GaugeHiggsUnification.WallDeterminants.neutral_three_det
{R : Type u_1}
[CommRing R]
(a b k d x y : R)
:
The neutral Gram determinant [[a x², a x y, −a d x], [a x y, a y² + b, −a d y], [−a d x, −a d y, a + k]]; b is the coefficient of the bulk field and k the total additional
hidden coefficient.
theorem
GaugeHiggsUnification.WallDeterminants.neutral_energy_decomposition
{R : Type u_1}
[CommRing R]
(a b k d x y u v w : R)
:
The neutral quadratic form as a sum of three weighted squares.